Belt drives systems may be assembled to (Figure 9.1): Opened belt drive (non-reversing) Reversing crossed or twist belt drive Angled belt drive
|
|
- Daniela Dorsey
- 7 years ago
- Views:
Transcription
1 heory of Machines / Belt Drives 9. Belt Drives 9. Geometry Specification 9.. Construction: Belt drives systems may be consist of (Figure 9.): Driving pulley Driven pulleys (multiple driven sources) Belts Idler and levers (used for adjustment) ω Smaller pulley v belt v Ω Opened belt drive Crossed belt drive Larger pulley Belt drives systems may be assembled to (Figure 9.): Opened belt drive (non-reversing) Reversing crossed or twist belt drive Angled belt drive Reversing open belt drive Angled belt drive Driver Driven Driven Multi output supplies here are many types of belts used these days, these are: Flat belt: used for moderate amount of power is to be transmitted. V-belt: greater amount of power is to be transmitted, and when the two pulleys are very near to each other. Circular Belt or Rope: greater amount of power is to be transmitted, and when the two pulleys are more than 5 m apart. iming belt: It has teeth that fit into groove cut on the periphery of the pulleys. A timing belt dose not stretches or slips and consequently transmits power at a constant angular velocity ratio, Figure 9.. belt Reversing open-belt belt drive drive Figure 9. Figure
2 heory of Machines / Belt Drives 9.. Angle of lap (contact), q: he belts are partly wound round pulleys. he smaller wound angle is called the Angle of lap or angle of contact. a. For opened belt drive: R, r radii of large and smaller pulleys respectively θ angle of lap S distance between pulley's centers Consider the triangle O O P (Figure 9.) O P R - r O O S cos (θ/) (R - r)/s θ cos - (R r)/s θ π/90* cos - (R r)/s in degree in radian If R r θ π rad 80 v P υ r υ/ R O O Ω b. For closed belt drive: Figure 9. Consider the triangle O O P (Figure 9.4) O P R + r O O S cos (ϕ/) (R + r)/s ϕ cos - (R + r)/s θ 60 - cos - (R + r)/s θ π/90* (80 - cos - (R + r)/s) in degree in radian - -
3 heory of Machines / Belt Drives P r θ ω/ R O v O Figure Length of the belt (L): a. For an opened belt drive: L rθ + R*(π - θ) + *(O P); O P S*sin θ/ L rθ + R*(π - θ) + *S*sin θ/ b. For a closed belt drive: L (R + r)θ + *(O P); O P S*sin ϕ/ S* sin (80 - θ/) L (R + r)θ + *S*sin (80 - θ/) 9..4 Speed Ratio of a Simple Belt Drive (e): a. If the larger pulley is the driver: e ω/ω R/r for no slipping and the thickness is not considered b. If smaller pulley is the driver: e Ω/ω r/r [ for no slipping and the thickness is not considered where Ω, and ω is the speed of the larger and smaller pulley in radian per second respectively Speed Ratio of a Compound Belt Drive (e): a. If the larger pulley is the driver and if there are four pulleys in the system: e ω/ω R *R /r *r 4 for no slipping and the thickness is not considered b. If smaller puller is the driver and if there are four pulleys in the system: e Ω/ω r *r /R *R 4 [ for no slipping and the thickness is not considered respectively Slip of belt Sometimes, the frictional grip becomes insufficient. his may cause some forward motion of the driver without carrying the belt with it. his may also cause some - -
4 heory of Machines / Belt Drives forward motion of the belt without carrying the driven pulley with it. his is called slip of the belt and is generally expressed as a percentage. he result of belt slipping is to reduce the velocity ratio of the system. Let s % Slip between the driver and the belt, s % Slip between the belt and the follower. v Velocity of the belt, passing over the driver per minute. d d ( s )( If thickness of the belt (t) is considered, then d d + t ( s + t )( s ) s ) Example : An engine, running at 50 rpm, drives a line shaft on the by means of a belt. he engine pulley is 75 cm diameter and the pulley on the line shaft being 45 cm. A 90 cm diameter pulley on the line shaft drives a 5 cm diameter pulley keyed to a dynamo shaft. Find the speed of the dynamo shaft, when,. there is no slip,. there is a slip of % at each drive. Given 50 rpm, D 75 cm, D 45 cm, D 90 cm, D 4 5 cm. When there is no slip: 4 4 * 4 D D D * D 50* rpm 4 75* 90 45* 5 0. When there is a slip of % at each drive 4 4 * 4 D D D * D ( s 50* rpm 4 )( s ) 75* 90 * ( 45* 5 00 )( 00 ) Example : Find the length of belt necessary to drive a pulley of 80 cm diameter running parallel at a distance of meters from the driving pulley of diameter 480 cm
5 heory of Machines / Belt Drives Given: R 40 cm, r 40 cm, S 00 cm. If the belt is open θ cos - (R r)/s cos - (40 40)/ rad L rθ + R*(π - θ) + *S*sin θ/ 40 * *(π ) +*00* cm. m. If the belt is crossed θ 60 - cos - (R + r)/s rad L (R + r)θ + *S*sin (80 - θ/) 45.8 cm.45 m 9. Ratio of Belt tensions: 9.. Flat Belt: Consider a flat belt partly wound round a pulley so that the angle of lap q, Figure 9.5, and let and be the tensions in the belt when it is about to slip in the direction shown. If the tensions at the ends of an element subtending an angle dq at the center are and + d, the reaction, and the coefficient of friction between the belt and the pulley is R and µ respectively, then resolving forces radially: dθ dθ ( + d ) + herefore, neglecting the second order of small quantities * dθ R Resolving forces tangentially, R (*) ight Side r Figure 9.5 Slack Side Figure
6 heory of Machines / Belt Drives ( + d ) d µ R µ dθ d ln µ dθ d µ θ µ R θ 0 µ dθ e µθ If the belt is used to transmit power between two pulleys, Figure 9.6, and are the tight and slack side tensions respectively. If the pulleys are unequal diameter, the belt will slip first on the pulley having the smaller angle of lap, i.e. on the smaller pulley. If v is the speed of the belt in m/s and and are in ewton, then Power transmitted ( )*v Watt *(-/e µq )*v Watt Example : Find the power transmitted by a belt running over a pulley of 60 cm diameter at 00 rpm. he coefficient of friction between the belt and the pulley is 0.5, angle of lap 60 and maximum tension in the belt is.5 k. Solution Given d 60 cm 0.6 m, 00 rpm, µ 0.5, q rad,.5 k v π*d*00/60 π m/s / e µq k Power transmitted ( )*v (.5.4) * π kw Example 4: wo pulleys, one 450 mm diameter and the mm diameter are on parallel shafts.95 m apart and are connected by crossed belt. Find the length of the belt required. What power the belt can transmit when the larger pulley rotates at 00 rpm, if the maximum permissible tension in the belt is k, and the coefficient between the belt and pulley is 0.5? other 00
7 heory of Machines / Belt Drives Given R 0.5 m, r 0. m, S.95 m, 00 rpm, k, µ 0.5. v π*r*00/ m/s q 60 - cos - (R + r)/s 60 - * cos - ( )/ rad L (R + r)q + *S*sin (80 - q/) ( )* *.95*sin ( ) m / e µq 000/e Power transmitted ( )*v ( )* W.76 kw 9.. Effect of Centrifugal ension: Consider a belt, of mass m per unit length, wound round a pulley of radius r, Figure 9.7. Let the speed of the belt be v and the centrifugal tension be c. Figure 9.7 If F is the centrifugal force acting on an element of the belt subtending an angle dθ at the center, then resolving forces radially, or dθ v F c i.e mrdθ. cdθ r c mv his is the tension caused by centrifugal force on the belt and is additional to the tension due to the transmission of power. Equation (*) due to this additional tension becomes: v dθ R + F R + mrdθ r So that d µ R µ ( - mv ) dθ d i.e. µdθ - c - 7 -
8 heory of Machines / Belt Drives or d c c c θ 0 µθ e µ dθ - c and - c are the effective driving tensions and and are now the total tensions in the belt. he transmitted power with the effects of centrifugal tension is; ( ) ν µ power ( )* v c θ e From the above equation the power transmitted is a maximum when d dv d dv mv c {( ) ν} c ( v mv ) 0 0 e Maximum power * * v µθ opt where v opt 9.. Initial ension: * m he belt is assembled with an initial tension, o. When power is being transmitted, the tension in the tight side increases from o to and on the slack side decreases from o to. o o or + o eglecting centrifugal tension 9. V Belt or Rope Drive 9.. Advantages and Disadvantages of V-belt Drive over Flat Belt Drive Advantages - 8 -
9 heory of Machines / Belt Drives. he V-belt drive gives compactness due to small distance between centers of pulleys.. he slip between the belt and the pulley groove is negligible.. he operation of the belt and pulley is quiet. 4. he high velocity ratio (maximum 0) may be obtained. 5. he power transmitted by V-belts is more than flat belts for the same coefficient of friction, arc of contact (angle of lap) and allowable tension in the belt. 6. he V-belt may be operated in either direction, with tight side of the β belt at top or bottom. he center line may be horizontal, vertical, or inclined. R V-belt Disadvantages. he V-belt drive cannot be used with large center distance.. he V-belts are not as durable as flat belts.. he construction of pulleys for V-belts is more complicated than pulleys of flat belts. β R/ 9.. Ratio of V-belt ensions: As in the flat belt drive, let tight tension in belt slack tension in belt R total reaction in the plane of the groove ormal reaction between belt and sides of the groove β angle of the groove µ coefficient of friction between the belt and sides of the groove From the force polygon in Figure 9.8, R sin β R cosecβ V-grooved pulley Figure 9.8 We have two friction forces, F µ * f \ F µ * R* cos ecβ f he friction force is therefore increased in the ratio cosecβ:, so that the V-grooved pulley is equivalent to a flat pulley having a coefficient of friction of µ.cosecβ. Hence - 9 -
10 heory of Machines / Belt Drives e µθ cos ec β When the effect of centrifugal tension is considered, the tension ratio became: - - c c µθ cos ecβ e Power ( ) * v ( C )* (-/e µθcosecβ )* v For the condition of maximum transmitted power, Maximum power e * * v µθ cosecβ opt where v opt * m Example 5: A belt drive consists of two V-belts in parallel, on grooved pulleys of the same size. he angle of the groove is 0. he cross-sectional area of each belt is 750 mm and µ 0.. he density of the belt material is. Mg/m and the maximum safe stress in the material is 7 M/m. Calculate the power that can be transmitted between pulleys 00 mm diameter rotating at 500 rpm. Find also the shaft speed in rpm at which the power transmitted would be a maximum. Given β 5, θ 80 π rad, µ 0., 500 rpm v π*r*/60.56 m/s We know that mass of the belt per meter length m area x density 750 x 0-6 x kg/m Centrifugal tension, c mv 0.9 x and maximum tension maximum stress x cross-sectional area of the belt 7 x 0 6 x 750 x ( c )/ ( c ) e µθ.cosecβ Power transmitted *( - ) * v 7.68 kw For maximum power, c / 750 mv 750 v (750/0.9) 0.5 v 44. m/s ω*r - 0 -
11 heory of Machines / Belt Drives ω 44./ rad/s 0* 94/π 807 rev/min Example 6: A rope drive is required to transmit 0 kw from a pulley of m diameter running at 450 rpm. he safe pull in each rope is 800 and the mass of the rope is 0.46 kg/m. he angle of lap and the groove angle are 60 and 45 respectively. If the coefficient of friction between the rope and the pulley is 0., find the number of ropes required. v π * d* /60.56 m/s c m* v 0.46 * ( c ) / ( c ) e µθ. cosecβ We know that power transmitted per rope; ( )* v.40 kw o. Of ropes otal power transmitted/ Power transmitted per rope 0/ or Example 7: An open belt drive connects two pulleys. and 0.5 m diameter, on parallel shafts.6 m apart. he belt has a mass of 0.9 kg/m length, and the maximum tension in it is not to exceed k. he. m pulley, which is the driver, runs at 00 rev/min. Due to belt slip on one of the pulleys, the velocity of the driven shaft is only 450 rev/min. Calculate the torque on each of the two shafts, the power transmitted, and the power lost in friction. µ 0.. What is the efficiency of the drive? From Figure 9.0, cos (θ/) ( )/ θ/ 84 5'.47 rad Angle of lap on smaller pulley, θ.994 rad he belt speed is that corresponding peripheral speed of the large (driving) pulley. v 00 * π * 0.6 / 0.57 m/s Figure to the
12 heory of Machines / Belt Drives C m * v 0.9 * c µθ e c 90 orque on driver ( ) * R (000 90) * m orque on follower ( ) * r (000 90) * m Power ( ) * v (000 90) * W.7 kw If there were no slip, speed of follower would be: ω speed ratio * Ω. * 00 / rev/min Power transmitted to follower.7 *450 / kw Power lost in friction kw Efficiency output power/ input power (.85 /.7) * % Example 8: A small air compressor is belt-driven from a lay shaft in a workshop, the pulley on the compressor being 00 mm diameter, and the angle of lap of the belt is 65. When the belt is moved from the loose to the fast pulley, it slips for 8 s until the compressor attains its constant speed of 00 rev/min. he flywheel of the compressor has a moment of inertia of 4 kg m and the friction requires a constant torque of 4 m. If the coefficient of friction is 0.8 during the accelerating period, find the tensions in both reaches of the belt, and also the distance that the belt slips and the energy lost in that time due to belt slip. θ 65 π*65/ rad ω π*00/60.46 rad/s While slip is taking place, ratio of belt tensions, / e µθ e 0.8* () Angular acceleration of compressor α dω/dt.46/8.97 rad/s et torque on compressor ( )* R 4 I * α (4 * ) / () herefore, from () and (): 7 and 06 Belt velocity v ω * R.46 * m/s Distance moved in 8 sec. 8 * m Distance moved by a point on the circumference 0.5 * m Slip of belt relative to pulley m Energy lost due to slip ( )* distance slipped.4 * J - -
13 heory of Machines / Belt Drives Example 9: wo parallel horizontal shafts, whose center lines are 4.8 m apart, one being vertically above the other, are connected by an open belt drive. he pulley on the upper shaft is.05 m diameter that on the lower shaft.5 m diameter. he belt is 50 mm wide and the initial tension in it when stationary and when no torque is being transmitted is k. he belt has a mass of.5 kg/m length; the gravitational force on it may be neglected but centrifugal force must be taken into account. he material of the belt may be assumed to obey Hook's Law, and the free lengths of the belt between pulleys may be assumed to be straight. he coefficient of friction between the belt and either pulley is 0.. Calculate a) he pressure in /m between the belt and the upper pulley when the belt and pulleys are stationary and no torque is being transmitted; b) he tension in the belt and the pressure between the belt and the upper pulley if the upper shaft rotates at 400 rev/min and there is no resisting torque on the lower shaft, hence no power being transmitted; c) he greatest tension in the belt in the belt if the upper shaft rotates at 400 rev/min and the maximum possible power is being transmitted to the shaft. υ 000 p dυ 000 (b) υ/ (a) Figure 9.0 a) Let the pressure on an element subtending an angle dθ at the center, Figure 9.0b, be p /m. hen, resolve forces radially. p * 0.55 * dθ * 0.5 * 000 * sin dθ/ p 800 /m b) v ω*r (π*400/60)* m/s C m*v.5 * Because part of the tension in this case is due to centrifugal tension, however, and the reaction between the belt and the pulley is reduced. - -
14 heory of Machines / Belt Drives Effective tension p 800 * 75/ /m c) cos (θ/) ( )/ θ 74 8'.05 rad + o 6000 () Also c µθ e e 0.*.05.5 () c herefore, from equations () and (), 970 Example 0: A compressor, requiring 90 kw, is to run at about 50 rpm. he drive is by V-belts from an electric motor running at 750 rpm. he diameter of the pulley on the compressor shaft must not be greater than m while the center distance between the pulleys is limited to.75 m. he belt speed should not exceed 600 m/min. Determine the number of V-belts required transmitting the power if each belt has a cross-sectional area of 75 mm, weighs 0.00 kg / cm, and has allowable tensile stress of.5 M / m. he groove angle of the pulley is 5. he coefficient of friction is 0.5. Calculate also the length required of each belt. Ω / ω r / R r 0.5 * 50/ m v 600 / m/s he weight of the belt per length, m ρ * A 0.00 * 0 6 * 75 * kg / m C m * v 0.75 * Maximum tension in the belt,.5 * 0 6 * A.5 * 0 6 * 75 * C For open belt drive, cos (θ/) ( )/ θ rad For V-belt drive, the ratio of belt tension with centrifugal effect taking into account, ( C ) / ( C ) e µθ.cosecβ e 0.5*.757*cosec (7.5) / he power transmitted by one belt, Power ( ) * v ( ) * W 6.94 kw - 4 -
15 heory of Machines / Belt Drives umber of V-belts 90 / belts Length of belt, * * (π -.757) + *.75 * sin m Example : An electric motor running at 400 rev/min transmits power by V-belts, each of 0 mm cross-sectional area, the total angle of groove being 45. he density of the belt material is.65 Mg/m and the maximum allowable working stress in the belts is M/m. µ 0.. he angle of lap on the motor pulley is 45. Calculate the maximum power, which can be transmitted, and the corresponding diameter of the motor pulley. ω π*400/ rad/s θ radians m ρ * A 650 * 0 * kg/m stress * A * 0 6 * 0 * In the maximum power condition, and or L rθ + R*(π - θ) + *S*sin θ/ C / 640 /. v opt ( /m) m/s e µθcosecβ e 0.*.507*cosec(.5).75 max. power (640.) * (-/.75) * 0. * 887 W 8.87 kw 8.9 kw Maximum power * e * v * 640* ( )* 0.*.75 Example : he following 887 W 8.87 kw data refer to an open belt drive: Diameter of larger pulley 400 mm Diameter of smaller pulley 50 mm Distance between two pulleys m Coefficient of friction 0.4 Maximum tension when the belt is on the point of slipping 00 Find the power transmitted at a speed of 0 m/s. It is desired to increase the power. Which of the following two methods you will select?. Increasing the initial tension in the belt by 0 %.. Increasing the coefficient of friction by 0 %. µθ cos ecβ opt * n - 5 -
16 heory of Machines / Belt Drives cos (θ/) (0. 0.5)/ θ radians / e µθ e 0.4* / o + o 776 power ( ) * v (00 5) * W 8.48 kw. power transmitted when the initial tension increased by 0 %: o * e µθ const o ( / +) * / (e µθ +) * power ( ) * v ( ) * W 9.8 kw. power transmitted when the coefficient of friction increased by 0 %: µ new * e 0.44* o 776 ( ) / * 776 / ( ) 9.7 and * power ( ) * v (. 9.7) * 0 96 W 9.6 kw Since the power transmitted by increasing the initial tension is more, therefore, we shall adopt the first method, i.e. increasing the initial tension. Example : A flat belt is required to transmit 5 kw from a pulley of.5 m effective diameter running at 00 rpm. he angle of contact is stretch over /4 of the circumference and the coefficient of friction between belt and pulley surface is 0.. Determine, taking centrifugal tension into account, width of the belt required. It is given that the belt thickness is 9.5 mm, density of its material is. Mg/m and the related permissible working stress is.5 /mm. θ 60 */ rad m ρ * t * b 00 * 9.5 * 0 - * b 0.45b kg/m v π*r*/60.56 m/s C m* v m 580.5b σ max * t * b.5 *0 6 * 9.5*0 - * b 750b Power transmitted: Power ( C )(-/e µθ )* v C Power /[(-/e µθ )* v] b b b b m 4 mm - 6 -
17 heory of Machines / Belt Drives Problems (Belt Drives) Q: wo shafts whose centers are 00 cm apart are connected by a V-belt drive. he driving pulley is supplied with 9.5 kw and has an effective diameter of 0. m. It runs at 000 rpm while the driven pulley runs at 75 rpm. he angle of groove on the pulleys is 40. Permissible tension in 4 cm cross-sectional area belt is. M/m. he material of the belt weighs. g/cm. he coefficient of friction between belt and pulley rim is 0.8. Estimate the number of belts required. (Ans. 0) Q: A leather belt, 5 mm wide and 6 mm thick, transmits power from a pulley 750 mm diameter which runs at 500 rev/min. he angle of lap is 50 and µ 0.. If the mass of m of leather is Mg and the stress in the belt is not to exceed.75 M/m, find the maximum power which can be transmitted. (Ans kw) Q: Power is transmitted between two shafts by a V-belt whose mass is 0.9 kg/m length. he maximum permissible tension in the belt is limited to. k. he angle of lap is 70 and the groove angle 45. If the coefficient of friction between the belt and pulleys is 0.7; find (i) velocity of the belt for maximum power; and (ii) power transmitted at this velocity. (Ans m/s; 0.66 kw) Q4: In a belt drive, the angle of lap of the belt on the small pulley is 50. With a belt speed of 0 m/s and a tension in the tight side of the belt of.5 k, the greatest power which can be transmitted without slip is 0 kw. What increase of power would be obtained for the same belt speed and maximum tension by using an idler pulley to increase the angle of lap to 0? ake into account the centrifugal effect, the mass of the belt being 0.75 kg/m. (Ans..6 kw) Q5: A pulley is driven by a flat belt, the angle of lap being 0. he belt is 00 mm wide by 6 mm thick and has a mass of Mg/m. If µ 0. and the maximum stress in the belt is not to exceed.5 M/m, find the greatest power which the belt can transmit and the corresponding speed of the belt. (Ans kw,.6 m/s) Q6: Power is transmitted between two shafts, 4.5 m apart, by a crossed wire rope passing round two pulleys, of m and m diameter respectively, the groove angle being 40. If the rope has a mass of 4 kg/m, and the maximum working tension is 0 k, determine the maximum power that the rope can transmit, and the corresponding speed of the smaller pulley. µ 0. (Ans kw, 89.9 rev/min) Q7: Power is transmitted from an electric motor to a machine tool by an open belt drive. he effective diameter of the pulley on the motor shaft is 50 mm while that on the machine tool is 00 mm with a center distance of 600 mm. If the motor speed is 440 rev/min and the maximum permissible belt tension is 900, then the maximum power transmissible is 6 kw. It is necessary that the power transmissible be increased to 6.75 kw, using the same pulleys, center distance and motor speed. he belt is treated with a special preparation - 7 -
18 heory of Machines / Belt Drives that increases its coefficient of friction by 0 percent of its existing value, and in addition a jockey pulley may be fitted. Determine, a) the existing coefficient of friction b) the new angle of lap (Ans. 0.9, 95 ) Q8: A belt drive consists of a V-belt working on a grooved pulley, with an angle lap of 60. he cross-sectional area of the belt is 650 mm, the groove angle is 0 and µ 0.. he density of the belt material is Mg/m and its maximum safe stress is 8 M/m of cross-section. Calculate the power that can be transmitted at a belt speed of 5 m/s. (Ans. 79 kw) Q9: he following particulars apply to one pulley of a rope drive between two parallel shafts: Effective diameter of pulley.5 m otal angle of groove 45 Minimum angle of lap 80 Mass of rope per m run 0.45 kg Maximum permitted load per rope 650 Coefficient of friction 0.5 a) Find the power transmitted per rope at a pulley speed of 00 rev/min, if centrifugal tension may be neglected. b) Find the pulley speed when centrifugal tension accounts for half the permitted load in the rope, and the power, which can be transmitted at that speed. (Ans. 8.9 kw, 4 rev/min, 7.6 kw) Q0: A /4 reduction drive between two parallel shafts m centers is provided by means of five parallel V-belts running on suitable pulleys mounted on the shafts. he effective diameter of the driving pulley is 50 mm and the driving shaft rotates at 740 rev/min. he included angle of each pulley groove is 40, each V-belt has a mass of 0.45 kg/m and the coefficient of friction between belt and each groove is 0.8. Determine what power can be transmitted by drive, if the tension in each belt is not to exceed 800. (Ans: 4.9 kw) Q: A small generator is driven by means of a V-belt which has a total angle of 60 between the faces of the V. he angle of lap on pulley is 0 and the mean radius of the belt as it passes round the pulley is 50 mm. If µ 0. and the mass of the belt is 0.45 kg/m, find the tension in each side of the belt when 750 Watt is being transmitted at a pulley speed of 800 rev/min. (Ans: 80 ; 00.5 ) Q: A shaft running at 00 rpm is to drive another shaft at 40 rpm and transmits kw. he distance between the shafts is 50 cm and the smaller pulley is of 60 cm diameter. he flat belt employed is 4 mm wide, mm thick, and the coefficient of - 8 -
19 heory of Machines / Belt Drives friction between the belt and pulley is 0.5. Calculate the stress in the belt if it is (a) an open belt drive; and (b) a cross belt drive
SOLID MECHANICS DYNAMICS TUTORIAL PULLEY DRIVE SYSTEMS. This work covers elements of the syllabus for the Edexcel module HNC/D Mechanical Principles.
SOLID MECHANICS DYNAMICS TUTORIAL PULLEY DRIVE SYSTEMS This work covers elements of the syllabus for the Edexcel module HNC/D Mechanical Principles. On completion of this tutorial you should be able to
More informationMechanical Principles
Unit 4: Mechanical Principles Unit code: F/60/450 QCF level: 5 Credit value: 5 OUTCOME 3 POWER TRANSMISSION TUTORIAL BELT DRIVES 3 Power Transmission Belt drives: flat and v-section belts; limiting coefficient
More informationBelt Drives and Chain Drives. Power Train. Power Train
Belt Drives and Chain Drives Material comes for Mott, 2002 and Kurtz, 1999 Power Train A power train transmits power from an engine or motor to the load. Some of the most common power trains include: Flexible
More informationMECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES
MECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES Simple machines: lifting devices e.g. lever systems, inclined plane, screw jack, pulley blocks, Weston differential
More informationCHAPTER 15 FORCE, MASS AND ACCELERATION
CHAPTER 5 FORCE, MASS AND ACCELERATION EXERCISE 83, Page 9. A car initially at rest accelerates uniformly to a speed of 55 km/h in 4 s. Determine the accelerating force required if the mass of the car
More informationProblem Set 1. Ans: a = 1.74 m/s 2, t = 4.80 s
Problem Set 1 1.1 A bicyclist starts from rest and after traveling along a straight path a distance of 20 m reaches a speed of 30 km/h. Determine her constant acceleration. How long does it take her to
More information3 Work, Power and Energy
3 Work, Power and Energy At the end of this section you should be able to: a. describe potential energy as energy due to position and derive potential energy as mgh b. describe kinetic energy as energy
More informationSOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS
SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS This work covers elements of the syllabus for the Engineering Council exams C105 Mechanical and Structural Engineering
More informationSOLID MECHANICS DYNAMICS TUTORIAL MOMENT OF INERTIA. This work covers elements of the following syllabi.
SOLID MECHANICS DYNAMICS TUTOIAL MOMENT OF INETIA This work covers elements of the following syllabi. Parts of the Engineering Council Graduate Diploma Exam D5 Dynamics of Mechanical Systems Parts of the
More informationUnit 4 Practice Test: Rotational Motion
Unit 4 Practice Test: Rotational Motion Multiple Guess Identify the letter of the choice that best completes the statement or answers the question. 1. How would an angle in radians be converted to an angle
More informationChapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.
Chapter 10 Rotational Motion Angular Quantities Units of Chapter 10 Vector Nature of Angular Quantities Constant Angular Acceleration Torque Rotational Dynamics; Torque and Rotational Inertia Solving Problems
More informationAngular acceleration α
Angular Acceleration Angular acceleration α measures how rapidly the angular velocity is changing: Slide 7-0 Linear and Circular Motion Compared Slide 7- Linear and Circular Kinematics Compared Slide 7-
More informationTorque and Rotary Motion
Torque and Rotary Motion Name Partner Introduction Motion in a circle is a straight-forward extension of linear motion. According to the textbook, all you have to do is replace displacement, velocity,
More informationPHYSICS 111 HOMEWORK SOLUTION #9. April 5, 2013
PHYSICS 111 HOMEWORK SOLUTION #9 April 5, 2013 0.1 A potter s wheel moves uniformly from rest to an angular speed of 0.16 rev/s in 33 s. Find its angular acceleration in radians per second per second.
More informationChapter 11. h = 5m. = mgh + 1 2 mv 2 + 1 2 Iω 2. E f. = E i. v = 4 3 g(h h) = 4 3 9.8m / s2 (8m 5m) = 6.26m / s. ω = v r = 6.
Chapter 11 11.7 A solid cylinder of radius 10cm and mass 1kg starts from rest and rolls without slipping a distance of 6m down a house roof that is inclined at 30 degrees (a) What is the angular speed
More informationChapter 4. Forces and Newton s Laws of Motion. continued
Chapter 4 Forces and Newton s Laws of Motion continued 4.9 Static and Kinetic Frictional Forces When an object is in contact with a surface forces can act on the objects. The component of this force acting
More informationMidterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m
Midterm Solutions I) A bullet of mass m moving at horizontal velocity v strikes and sticks to the rim of a wheel a solid disc) of mass M, radius R, anchored at its center but free to rotate i) Which of
More informationENGINEERING COUNCIL CERTIFICATE LEVEL ENGINEERING SCIENCE C103 TUTORIAL 3 - TORSION
ENGINEEING COUNCI CETIFICATE EVE ENGINEEING SCIENCE C10 TUTOIA - TOSION You should judge your progress by completing the self assessment exercises. These may be sent for marking or you may request copies
More informationLecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is
Lecture 17 Rotational Dynamics Rotational Kinetic Energy Stress and Strain and Springs Cutnell+Johnson: 9.4-9.6, 10.1-10.2 Rotational Dynamics (some more) Last time we saw that the rotational analog of
More informationCentripetal Force. This result is independent of the size of r. A full circle has 2π rad, and 360 deg = 2π rad.
Centripetal Force 1 Introduction In classical mechanics, the dynamics of a point particle are described by Newton s 2nd law, F = m a, where F is the net force, m is the mass, and a is the acceleration.
More informationwww.mathsbox.org.uk Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x
Mechanics 2 : Revision Notes 1. Kinematics and variable acceleration Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx differentiate a = dv = d2 x dt dt dt 2 Acceleration Velocity
More informationSolution Derivations for Capa #11
Solution Derivations for Capa #11 1) A horizontal circular platform (M = 128.1 kg, r = 3.11 m) rotates about a frictionless vertical axle. A student (m = 68.3 kg) walks slowly from the rim of the platform
More informationPhysics 201 Homework 8
Physics 201 Homework 8 Feb 27, 2013 1. A ceiling fan is turned on and a net torque of 1.8 N-m is applied to the blades. 8.2 rad/s 2 The blades have a total moment of inertia of 0.22 kg-m 2. What is the
More informationSOLID MECHANICS DYNAMICS TUTORIAL CENTRIPETAL FORCE
SOLID MECHANICS DYNAMICS TUTORIAL CENTRIPETAL FORCE This work coers elements of the syllabus for the Engineering Council Exam D5 Dynamics of Mechanical Systems C10 Engineering Science. This tutorial examines
More informationB.TECH. (AEROSPACE ENGINEERING) PROGRAMME (BTAE) Term-End Examination December, 2011 BAS-010 : MACHINE DESIGN
No. of Printed Pages : 7 BAS-01.0 B.TECH. (AEROSPACE ENGINEERING) PROGRAMME (BTAE) CV CA CV C:) O Term-End Examination December, 2011 BAS-010 : MACHINE DESIGN Time : 3 hours Maximum Marks : 70 Note : (1)
More informationChapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces. Copyright 2009 Pearson Education, Inc.
Chapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces Units of Chapter 5 Applications of Newton s Laws Involving Friction Uniform Circular Motion Kinematics Dynamics of Uniform Circular
More informationAcceleration due to Gravity
Acceleration due to Gravity 1 Object To determine the acceleration due to gravity by different methods. 2 Apparatus Balance, ball bearing, clamps, electric timers, meter stick, paper strips, precision
More informationCenter of Gravity. We touched on this briefly in chapter 7! x 2
Center of Gravity We touched on this briefly in chapter 7! x 1 x 2 cm m 1 m 2 This was for what is known as discrete objects. Discrete refers to the fact that the two objects separated and individual.
More information11. Rotation Translational Motion: Rotational Motion:
11. Rotation Translational Motion: Motion of the center of mass of an object from one position to another. All the motion discussed so far belongs to this category, except uniform circular motion. Rotational
More informationPHY121 #8 Midterm I 3.06.2013
PHY11 #8 Midterm I 3.06.013 AP Physics- Newton s Laws AP Exam Multiple Choice Questions #1 #4 1. When the frictionless system shown above is accelerated by an applied force of magnitude F, the tension
More informationCE 3500 Fluid Mechanics / Fall 2014 / City College of New York
1 Drag Coefficient The force ( F ) of the wind blowing against a building is given by F=C D ρu 2 A/2, where U is the wind speed, ρ is density of the air, A the cross-sectional area of the building, and
More informationPHYS 211 FINAL FALL 2004 Form A
1. Two boys with masses of 40 kg and 60 kg are holding onto either end of a 10 m long massless pole which is initially at rest and floating in still water. They pull themselves along the pole toward each
More informationSo if ω 0 increases 3-fold, the stopping angle increases 3 2 = 9-fold.
Name: MULTIPLE CHOICE: Questions 1-11 are 5 points each. 1. A safety device brings the blade of a power mower from an angular speed of ω 1 to rest in 1.00 revolution. At the same constant angular acceleration,
More informationLab 7: Rotational Motion
Lab 7: Rotational Motion Equipment: DataStudio, rotary motion sensor mounted on 80 cm rod and heavy duty bench clamp (PASCO ME-9472), string with loop at one end and small white bead at the other end (125
More informationLecture Presentation Chapter 7 Rotational Motion
Lecture Presentation Chapter 7 Rotational Motion Suggested Videos for Chapter 7 Prelecture Videos Describing Rotational Motion Moment of Inertia and Center of Gravity Newton s Second Law for Rotation Class
More informationModule 2 - GEARS Lecture 7 - SPUR GEAR DESIGN
Module 2 - GEARS Lecture 7 - SPUR GEAR DESIGN Contents 7.1 Spur gear tooth force analysis 7.2 Spur gear - tooth stresses 7.3 Tooth bending stress Lewis equation 7.4 Tooth bending stress AGMA procedure
More informationAP Physics Circular Motion Practice Test B,B,B,A,D,D,C,B,D,B,E,E,E, 14. 6.6m/s, 0.4 N, 1.5 m, 6.3m/s, 15. 12.9 m/s, 22.9 m/s
AP Physics Circular Motion Practice Test B,B,B,A,D,D,C,B,D,B,E,E,E, 14. 6.6m/s, 0.4 N, 1.5 m, 6.3m/s, 15. 12.9 m/s, 22.9 m/s Answer the multiple choice questions (2 Points Each) on this sheet with capital
More informationPHY231 Section 2, Form A March 22, 2012. 1. Which one of the following statements concerning kinetic energy is true?
1. Which one of the following statements concerning kinetic energy is true? A) Kinetic energy can be measured in watts. B) Kinetic energy is always equal to the potential energy. C) Kinetic energy is always
More informationElectric Motors and Drives
EML 2322L MAE Design and Manufacturing Laboratory Electric Motors and Drives To calculate the peak power and torque produced by an electric motor, you will need to know the following: Motor supply voltage,
More informationPHYSICS 111 HOMEWORK SOLUTION #10. April 8, 2013
PHYSICS HOMEWORK SOLUTION #0 April 8, 203 0. Find the net torque on the wheel in the figure below about the axle through O, taking a = 6.0 cm and b = 30.0 cm. A torque that s produced by a force can be
More informationPHY231 Section 1, Form B March 22, 2012
1. A car enters a horizontal, curved roadbed of radius 50 m. The coefficient of static friction between the tires and the roadbed is 0.20. What is the maximum speed with which the car can safely negotiate
More informationPhysics 41 HW Set 1 Chapter 15
Physics 4 HW Set Chapter 5 Serway 8 th OC:, 4, 7 CQ: 4, 8 P: 4, 5, 8, 8, 0, 9,, 4, 9, 4, 5, 5 Discussion Problems:, 57, 59, 67, 74 OC CQ P: 4, 5, 8, 8, 0, 9,, 4, 9, 4, 5, 5 Discussion Problems:, 57, 59,
More informationColumbia University Department of Physics QUALIFYING EXAMINATION
Columbia University Department of Physics QUALIFYING EXAMINATION Monday, January 13, 2014 1:00PM to 3:00PM Classical Physics Section 1. Classical Mechanics Two hours are permitted for the completion of
More informationEXPERIMENT: MOMENT OF INERTIA
OBJECTIVES EXPERIMENT: MOMENT OF INERTIA to familiarize yourself with the concept of moment of inertia, I, which plays the same role in the description of the rotation of a rigid body as mass plays in
More informationLecture L5 - Other Coordinate Systems
S. Widnall, J. Peraire 16.07 Dynamics Fall 008 Version.0 Lecture L5 - Other Coordinate Systems In this lecture, we will look at some other common systems of coordinates. We will present polar coordinates
More informationTips For Selecting DC Motors For Your Mobile Robot
Tips For Selecting DC Motors For Your Mobile Robot By AJ Neal When building a mobile robot, selecting the drive motors is one of the most important decisions you will make. It is a perfect example of an
More informationAwell-known lecture demonstration1
Acceleration of a Pulled Spool Carl E. Mungan, Physics Department, U.S. Naval Academy, Annapolis, MD 40-506; mungan@usna.edu Awell-known lecture demonstration consists of pulling a spool by the free end
More informationRotational Motion: Moment of Inertia
Experiment 8 Rotational Motion: Moment of Inertia 8.1 Objectives Familiarize yourself with the concept of moment of inertia, I, which plays the same role in the description of the rotation of a rigid body
More informationRotational Inertia Demonstrator
WWW.ARBORSCI.COM Rotational Inertia Demonstrator P3-3545 BACKGROUND: The Rotational Inertia Demonstrator provides an engaging way to investigate many of the principles of angular motion and is intended
More informationPHYS 101-4M, Fall 2005 Exam #3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
PHYS 101-4M, Fall 2005 Exam #3 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A bicycle wheel rotates uniformly through 2.0 revolutions in
More informationLecture L22-2D Rigid Body Dynamics: Work and Energy
J. Peraire, S. Widnall 6.07 Dynamics Fall 008 Version.0 Lecture L - D Rigid Body Dynamics: Work and Energy In this lecture, we will revisit the principle of work and energy introduced in lecture L-3 for
More informationANALYTICAL METHODS FOR ENGINEERS
UNIT 1: Unit code: QCF Level: 4 Credit value: 15 ANALYTICAL METHODS FOR ENGINEERS A/601/1401 OUTCOME - TRIGONOMETRIC METHODS TUTORIAL 1 SINUSOIDAL FUNCTION Be able to analyse and model engineering situations
More information3600 s 1 h. 24 h 1 day. 1 day
Week 7 homework IMPORTANT NOTE ABOUT WEBASSIGN: In the WebAssign versions of these problems, various details have been changed, so that the answers will come out differently. The method to find the solution
More informationRotation: Moment of Inertia and Torque
Rotation: Moment of Inertia and Torque Every time we push a door open or tighten a bolt using a wrench, we apply a force that results in a rotational motion about a fixed axis. Through experience we learn
More informationMachine Design II Prof. K.Gopinath & Prof. M.M.Mayuram. Module 2 - GEARS. Lecture 17 DESIGN OF GEARBOX
Module 2 - GEARS Lecture 17 DESIGN OF GEARBOX Contents 17.1 Commercial gearboxes 17.2 Gearbox design. 17.1 COMMERCIAL GEARBOXES Various commercial gearbox designs are depicted in Fig. 17.1 to 17.10. These
More informationGear Trains. Introduction:
Gear Trains Introduction: Sometimes, two or more gears are made to mesh with each other to transmit power from one shaft to another. Such a combination is called gear train or train of toothed wheels.
More informationUniform Circular Motion III. Homework: Assignment (1-35) Read 5.4, Do CONCEPT QUEST #(8), Do PROBS (20, 21) Ch. 5 + AP 1997 #2 (handout)
Double Date: Objective: Uniform Circular Motion II Uniform Circular Motion III Homework: Assignment (1-35) Read 5.4, Do CONCEPT QUEST #(8), Do PROBS (20, 21) Ch. 5 + AP 1997 #2 (handout) AP Physics B
More informationPhysics 11 Assignment KEY Dynamics Chapters 4 & 5
Physics Assignment KEY Dynamics Chapters 4 & 5 ote: for all dynamics problem-solving questions, draw appropriate free body diagrams and use the aforementioned problem-solving method.. Define the following
More informationTechnology Exploration-I
Technology Exploration-I PREPARED BY Academic Services August 2011 Applied Technology High Schools, 2011 Module Objectives After the completion of this module, the student should be able to: Identify pulleys.
More informationWeight The weight of an object is defined as the gravitational force acting on the object. Unit: Newton (N)
Gravitational Field A gravitational field as a region in which an object experiences a force due to gravitational attraction Gravitational Field Strength The gravitational field strength at a point in
More informationC B A T 3 T 2 T 1. 1. What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N
Three boxes are connected by massless strings and are resting on a frictionless table. Each box has a mass of 15 kg, and the tension T 1 in the right string is accelerating the boxes to the right at a
More informationHW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions
HW Set VI page 1 of 9 10-30 A 10 g bullet moving directly upward at 1000 m/s strikes and passes through the center of mass of a 5.0 kg block initially at rest (Fig. 10-33 ). The bullet emerges from the
More informationENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 1 LINEAR AND ANGULAR DISPLACEMENT, VELOCITY AND ACCELERATION
ENGINEERING COUNCIL DYNAMICS OF MECHANICAL SYSTEMS D225 TUTORIAL 1 LINEAR AND ANGULAR DISPLACEMENT, VELOCITY AND ACCELERATION This tutorial covers pre-requisite material and should be skipped if you are
More informationAnswer, Key Homework 7 David McIntyre 45123 Mar 25, 2004 1
Answer, Key Hoework 7 David McIntyre 453 Mar 5, 004 This print-out should have 4 questions. Multiple-choice questions ay continue on the next colun or page find all choices before aking your selection.
More informationUseful Motor/Torque Equations for EML2322L
Useful Motor/Torque Equations for EML2322L Force (Newtons) F = m x a m = mass (kg) a = acceleration (m/s 2 ) Motor Torque (Newton-meters) T = F x d F = force (Newtons) d = moment arm (meters) Power (Watts)
More informationFluid Mechanics: Static s Kinematics Dynamics Fluid
Fluid Mechanics: Fluid mechanics may be defined as that branch of engineering science that deals with the behavior of fluid under the condition of rest and motion Fluid mechanics may be divided into three
More informationServo Motor Selection Flow Chart
Servo otor Selection Flow Chart START Selection Has the machine Been Selected? YES NO Explanation References etermine the size, mass, coefficient of friction, and external forces of all the moving part
More informationPhysical Quantities, Symbols and Units
Table 1 below indicates the physical quantities required for numerical calculations that are included in the Access 3 Physics units and the Intermediate 1 Physics units and course together with the SI
More informationWork, Power, Energy Multiple Choice. PSI Physics. Multiple Choice Questions
Work, Power, Energy Multiple Choice PSI Physics Name Multiple Choice Questions 1. A block of mass m is pulled over a distance d by an applied force F which is directed in parallel to the displacement.
More informationTennessee State University
Tennessee State University Dept. of Physics & Mathematics PHYS 2010 CF SU 2009 Name 30% Time is 2 hours. Cheating will give you an F-grade. Other instructions will be given in the Hall. MULTIPLE CHOICE.
More informationPractice Exam Three Solutions
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01T Fall Term 2004 Practice Exam Three Solutions Problem 1a) (5 points) Collisions and Center of Mass Reference Frame In the lab frame,
More informationv v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )
Week 3 homework IMPORTANT NOTE ABOUT WEBASSIGN: In the WebAssign versions of these problems, various details have been changed, so that the answers will come out differently. The method to find the solution
More informationFLUID MECHANICS. TUTORIAL No.7 FLUID FORCES. When you have completed this tutorial you should be able to. Solve forces due to pressure difference.
FLUID MECHANICS TUTORIAL No.7 FLUID FORCES When you have completed this tutorial you should be able to Solve forces due to pressure difference. Solve problems due to momentum changes. Solve problems involving
More informationMechanical Principles
Unit 4: Mechanical Principles Unit code: F/601/1450 QCF level: 5 Credit value: 15 OUTCOME 4 POWER TRANSMISSION TUTORIAL 2 BALANCING 4. Dynamics of rotating systems Single and multi-link mechanisms: slider
More informationLecture-IV. Contact forces & Newton s laws of motion
Lecture-IV Contact forces & Newton s laws of motion Contact forces: Force arises from interaction between two bodies. By contact forces we mean the forces which are transmitted between bodies by short-range
More informationPhysics 1A Lecture 10C
Physics 1A Lecture 10C "If you neglect to recharge a battery, it dies. And if you run full speed ahead without stopping for water, you lose momentum to finish the race. --Oprah Winfrey Static Equilibrium
More informationMercury is poured into a U-tube as in Figure (14.18a). The left arm of the tube has crosssectional
Chapter 14 Fluid Mechanics. Solutions of Selected Problems 14.1 Problem 14.18 (In the text book) Mercury is poured into a U-tube as in Figure (14.18a). The left arm of the tube has crosssectional area
More informationTorsion Tests. Subjects of interest
Chapter 10 Torsion Tests Subjects of interest Introduction/Objectives Mechanical properties in torsion Torsional stresses for large plastic strains Type of torsion failures Torsion test vs.tension test
More informationMotor Selection and Sizing
Motor Selection and Sizing Motor Selection With each application, the drive system requirements greatly vary. In order to accommodate this variety of needs, Aerotech offers five types of motors. Motors
More informationSimple Harmonic Motion
Simple Harmonic Motion 1 Object To determine the period of motion of objects that are executing simple harmonic motion and to check the theoretical prediction of such periods. 2 Apparatus Assorted weights
More information8.012 Physics I: Classical Mechanics Fall 2008
MIT OpenCourseWare http://ocw.mit.edu 8.012 Physics I: Classical Mechanics Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. MASSACHUSETTS INSTITUTE
More informationSOLUTIONS TO CONCEPTS CHAPTER 15
SOLUTIONS TO CONCEPTS CHAPTER 15 1. v = 40 cm/sec As velocity of a wave is constant location of maximum after 5 sec = 40 5 = 00 cm along negative x-axis. [(x / a) (t / T)]. Given y = Ae a) [A] = [M 0 L
More informationChapter 8: Rotational Motion of Solid Objects
Chapter 8: Rotational Motion of Solid Objects 1. An isolated object is initially spinning at a constant speed. Then, although no external forces act upon it, its rotational speed increases. This must be
More informationAP Physics - Chapter 8 Practice Test
AP Physics - Chapter 8 Practice Test Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A single conservative force F x = (6.0x 12) N (x is in m) acts on
More informationChapter 3.8 & 6 Solutions
Chapter 3.8 & 6 Solutions P3.37. Prepare: We are asked to find period, speed and acceleration. Period and frequency are inverses according to Equation 3.26. To find speed we need to know the distance traveled
More informationSOLID MECHANICS BALANCING TUTORIAL BALANCING OF ROTATING BODIES
SOLID MECHANICS BALANCING TUTORIAL BALANCING OF ROTATING BODIES This work covers elements of the syllabus for the Edexcel module 21722P HNC/D Mechanical Principles OUTCOME 4. On completion of this tutorial
More informationIf you put the same book on a tilted surface the normal force will be less. The magnitude of the normal force will equal: N = W cos θ
Experiment 4 ormal and Frictional Forces Preparation Prepare for this week's quiz by reviewing last week's experiment Read this week's experiment and the section in your textbook dealing with normal forces
More information9. The kinetic energy of the moving object is (1) 5 J (3) 15 J (2) 10 J (4) 50 J
1. If the kinetic energy of an object is 16 joules when its speed is 4.0 meters per second, then the mass of the objects is (1) 0.5 kg (3) 8.0 kg (2) 2.0 kg (4) 19.6 kg Base your answers to questions 9
More informationD Alembert s principle and applications
Chapter 1 D Alembert s principle and applications 1.1 D Alembert s principle The principle of virtual work states that the sum of the incremental virtual works done by all external forces F i acting in
More informationHand Held Centripetal Force Kit
Hand Held Centripetal Force Kit PH110152 Experiment Guide Hand Held Centripetal Force Kit INTRODUCTION: This elegantly simple kit provides the necessary tools to discover properties of rotational dynamics.
More informationINSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS
INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS This is a stand alone tutorial on electric motors and actuators. The tutorial is of interest to any student studying control systems and in particular
More informationDesign of a Rope Brake Dynamometer
Middle-East Journal of Scientific Research 0 (5): 650-655, 014 ISSN 1990-933 IDOSI Publications, 014 DOI: 10.589/idosi.mejsr.014.0.05.11356 Design of a Rope Brake Dynamometer R. Gopinath Department of
More informationObjective: To distinguish between degree and radian measure, and to solve problems using both.
CHAPTER 3 LESSON 1 Teacher s Guide Radian Measure AW 3.2 MP 4.1 Objective: To distinguish between degree and radian measure, and to solve problems using both. Prerequisites Define the following concepts.
More informationSolution: Angular velocity in consistent units (Table 8.1): 753.8. Velocity of a point on the disk: Rate at which bits pass by the read/write head:
Problem P8: The disk in a computer hard drive spins at 7200 rpm At the radius of 0 mm, a stream of data is magnetically written on the disk, and the spacing between data bits is 25 μm Determine the number
More informationPhysics 231 Lecture 15
Physics 31 ecture 15 Main points of today s lecture: Simple harmonic motion Mass and Spring Pendulum Circular motion T 1/f; f 1/ T; ω πf for mass and spring ω x Acos( ωt) v ωasin( ωt) x ax ω Acos( ωt)
More informationChapter 16. Mensuration of Cylinder
335 Chapter 16 16.1 Cylinder: A solid surface generated by a line moving parallel to a fixed line, while its end describes a closed figure in a plane is called a cylinder. A cylinder is the limiting case
More informationThere are four types of friction, they are 1).Static friction 2) Dynamic friction 3) Sliding friction 4) Rolling friction
2.3 RICTION The property by virtue of which a resisting force is created between two rough bodies that resists the sliding of one body over the other is known as friction. The force that always opposes
More informationPhysics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam
Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam INSTRUCTIONS: Use a pencil #2 to fill your scantron. Write your code number and bubble it in under "EXAM NUMBER;" an entry
More informationWork Energy & Power. September 2000 Number 05. 1. Work If a force acts on a body and causes it to move, then the force is doing work.
PhysicsFactsheet September 2000 Number 05 Work Energy & Power 1. Work If a force acts on a body and causes it to move, then the force is doing work. W = Fs W = work done (J) F = force applied (N) s = distance
More information